Ghosts in the Machine
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Catholic Christian Christian
Religious Scientists (From the Vatican Observatory Website) https://www.vofoundation.org/faith-and-science/religious-scientists/ Many scientists are religious people—men and women of faith—believers in God. This section features some of the religious scientists who appear in different entries on these Faith and Science pages. Some of these scientists are well-known, others less so. Many are Catholic, many are not. Most are Christian, but some are not. Some of these scientists of faith have lived saintly lives. Many scientists who are faith-full tend to describe science as an effort to understand the works of God and thus to grow closer to God. Quite a few describe their work in science almost as a duty they have to seek to improve the lives of their fellow human beings through greater understanding of the world around them. But the people featured here are featured because they are scientists, not because they are saints (even when they are, in fact, saints). Scientists tend to be creative, independent-minded and confident of their ideas. We also maintain a longer listing of scientists of faith who may or may not be discussed on these Faith and Science pages—click here for that listing. Agnesi, Maria Gaetana (1718-1799) Catholic Christian A child prodigy who obtained education and acclaim for her abilities in math and physics, as well as support from Pope Benedict XIV, Agnesi would write an early calculus textbook. She later abandoned her work in mathematics and physics and chose a life of service to those in need. Click here for Vatican Observatory Faith and Science entries about Maria Gaetana Agnesi. -
Beta Decay Introduction
Beta decay Introduction Beta decay is the decay mechanism that affects the largest number of nuclei. In standard beta decay, or more specifically, beta-minus decay, a nucleus converts a neutron into a proton. The number of neutrons N decreases by one unit, and the number of protons Z increases by one. So the neutron excess decreases by two. Beta decay moves nuclei with too many neutrons closer to the stable range. Unlike the neutron, the proton has a positive charge, so by itself, converting a neutron into a proton would create charge out of nothing. However, that is not possible as net charge is preserved in nature. In beta decay, the nucleus also emits a negatively charged electron, making the net charge that is cre- ated zero as it should. But there is another problem with that. Now a neutron with spin 1/2 is converted into a proton and an electron, each with spin 1/2. That violates angular momentum conservation. (Regardless of any orbital angular momentum, the net angular momentum would change from half-integer to integer.) In beta de- cay, the nucleus also emits a second particle of spin 1/2, thus keeping the net angular momentum half- integer. Fermi called that second particle the neutrino, since it was electrically neutral and so small that it was initially impossible to observe. In fact, even at the time of writing, almost a century later, the mass of the neutrino, though known to be nonzero, is too small to measure. Nowadays the neutrino emitted in beta decay is more accurately identified as the electron antineutrino. -
Realization of the Low Background Neutrino Detector Double Chooz: from the Development of a High-Purity Liquid & Gas Handling Concept to first Neutrino Data
Realization of the low background neutrino detector Double Chooz: From the development of a high-purity liquid & gas handling concept to first neutrino data Dissertation of Patrick Pfahler TECHNISCHE UNIVERSITAT¨ MUNCHEN¨ Physik Department Lehrstuhl f¨urexperimentelle Astroteilchenphysik / E15 Univ.-Prof. Dr. Lothar Oberauer Realization of the low background neutrino detector Double Chooz: From the development of high-purity liquid- & gas handling concept to first neutrino data Dipl. Phys. (Univ.) Patrick Pfahler Vollst¨andigerAbdruck der von der Fakult¨atf¨urPhysik der Technischen Universit¨atM¨unchen zur Erlangung des akademischen Grades eines Doktors des Naturwissenschaften (Dr. rer. nat) genehmigten Dissertation. Vorsitzender: Univ.-Prof. Dr. Alejandro Ibarra Pr¨uferder Dissertation: 1. Univ.-Prof. Dr. Lothar Oberauer 2. Priv.-Doz. Dr. Andreas Ulrich Die Dissertation wurde am 3.12.2012 bei der Technischen Universit¨atM¨unchen eingereicht und durch die Fakult¨atf¨urPhysik am 17.12.2012 angenommen. 2 Contents Contents i Introduction 1 I The Neutrino Disappearance Experiment Double Chooz 5 1 Neutrino Oscillation and Flavor Mixing 6 1.1 PMNS Matrix . 6 1.2 Flavor Mixing and Neutrino Oscillations . 7 1.2.1 Survival Probability of Reactor Neutrinos . 9 1.2.2 Neutrino Masses and Mass Hierarchy . 12 2 Reactor Neutrinos 14 2.1 Neutrino Production in Nuclear Power Cores . 14 2.2 Energy Spectrum of Reactor neutrinos . 15 2.3 Neutrino Flux Approximation . 16 3 The Double Chooz Experiment 19 3.1 The Double Chooz Collaboration . 19 3.2 Experimental Site: Commercial Nuclear Power Plant in Chooz . 20 3.3 Physics Program and Experimental Concept . 21 3.4 Signal . 23 3.4.1 The Inverse Beta Decay (IBD) . -
Results in Neutrino Oscillations from Super-Kamiokande I
Status of the RENO Reactor Neutrino Experiment RENO = Reactor Experiment for Neutrino Oscillation (For RENO Collaboration) K.K. Joo Chonnam National University February 15, 2011 Research Techniques Seminar @FNAL Outline Experiment Goals of the RENO Exp. - Short introduction - Expected q13 sensitivity - Systematic uncertainty Overview of the RENO Experiment - Experimental Setup of RENO - Schedule - Tunnel excavation - Status of detector construction - DAQ, data analysis tools Summary Brief History of Neutrinos 1930: Pauli postulated neutrino to explain b decay problem 1933: Fermi baptized the neutrino in his weak-interaction theory 1956: First discovery of neutrino by Reines & Cowan from reactor 1957: Neutrinos are left-handed by Glodhaber et al. 1962: Discovery of nm by Lederman et al. (Brookhaven Lab) 1974: Discovery of neutral currents due to neutrinos 1977: Tau lepton discovery by Perl et al. (SLAC) 1998: Atmospheric neutrino oscillation observed by Super-K 2000: nt discovery by DONUT (Fermilab) 2002: Solar neutrino oscillation observed by SNO and confirmed by Kamland What NEXT? Standard Model Neutrinos in SM Neutrino Oscillation . Three types of neutrinos exist & mixing among them Oscillation parameters (q12 , q23 , q13) Not measured yet . Elementary particles with almost no interactions . Almost massless: impossible to measure its mass Neutrino Mixing Parameters Matrix Components: νe Ue1 Ue2 Ue3 ν1 3 Angles (θ ; θ ; θ ) 12 13 23 ν U U U ν 1 CP phase (δ) μ μ1 μ2 μ3 2 2 Mass differences ντ Uτ1 Uτ2 Uτ3 ν3 1 0 0 c 0 s ei c s 0 13 13 12 12 U 0 c23 s23 0 1 0 s12 c12 0 i 0 s23 c23 s13e 0 c13 0 0 1 atmospheric SK, K2K The Next Big Thing? SNO, solar SK, KamLAND ≈ ≈ ° q23 qatm 45 q12 ≈qsol ≈ 32° Large and maximal mixing! Reduction of reactor neutrinos due to oscillations Disappearance Reactor neutrino disappearance Prob. -
Neutrino Mysteries OLLI UC Irvine April 7, 2014
Neutrino Mysteries OLLI UC Irvine April 7, 2014 Dennis Silverman Department of Physics and Astronomy UC Irvine Neutrinos Around the Universe • Neutrinos • The Standard Model • The Weak Interactions Neutrino Oscillations • Solar Neutrinos • Atmospheric Neutrinos • Neutrino Masses • Neutrino vs. Antineutrino • Supernova Neutrinos Introduction to the Standard Model www.particleadventure.org Over 100 Years of Subatomic Physics Atoms to Electrons and Nuclei to Protons and Neutrons and to Quarks The size of a proton is about 10⁻¹³ cm, called a fermi. Protons have two up quarks and one down quark. Neutrons have one up quark and two down quarks. The Standard Model of Quarks and Leptons Electromagnetic, Weak, and Strong Color Interactions Q = +2/3 e Q = -1/3 e Q = 0 Q = - e The Spin of Particles, Charges, and Anti-particles • The quarks and leptons all have an intrinsic spin of ½ in units of hbar = h/2휋 =ħ, a very small number. These are called fermions after Enrico Fermi. They have anti-particles with opposite charges. • The up quarks have charge +2/3 of that of the electron’s magnitude, and the bottom quarks have charge -1/3. • The force particles have spin 1 times ħ, and are called bosons after S. N. Bose. • The force particles are their own antiparticles like Z⁰ and the photon, or in opposite pairs, like W⁺ and W⁻, and the colored gluons. Masses of Elementary Particles 125 GeV → The Proton and Neutron are about 1 GeV → A GeV is a giga electron volts in energy, or a billion electron volts Diagram from Gordon Kane, Scientific American 2003 The Weak Interactions The Beta (electron) Decay of a neutron is really that of a down quark to an up quark with a virtual W⁻ creating an electron and an electron anti-neutrino. -
Phase Transitions and the Casimir Effect in Neutron Stars
University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Masters Theses Graduate School 12-2017 Phase Transitions and the Casimir Effect in Neutron Stars William Patrick Moffitt University of Tennessee, Knoxville, [email protected] Follow this and additional works at: https://trace.tennessee.edu/utk_gradthes Part of the Other Physics Commons Recommended Citation Moffitt, William Patrick, "Phase Transitions and the Casimir Effect in Neutron Stars. " Master's Thesis, University of Tennessee, 2017. https://trace.tennessee.edu/utk_gradthes/4956 This Thesis is brought to you for free and open access by the Graduate School at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Masters Theses by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. To the Graduate Council: I am submitting herewith a thesis written by William Patrick Moffitt entitled "Phaser T ansitions and the Casimir Effect in Neutron Stars." I have examined the final electronic copy of this thesis for form and content and recommend that it be accepted in partial fulfillment of the requirements for the degree of Master of Science, with a major in Physics. Andrew W. Steiner, Major Professor We have read this thesis and recommend its acceptance: Marianne Breinig, Steve Johnston Accepted for the Council: Dixie L. Thompson Vice Provost and Dean of the Graduate School (Original signatures are on file with official studentecor r ds.) Phase Transitions and the Casimir Effect in Neutron Stars A Thesis Presented for the Master of Science Degree The University of Tennessee, Knoxville William Patrick Moffitt December 2017 Abstract What lies at the core of a neutron star is still a highly debated topic, with both the composition and the physical interactions in question. -
Melvin Schwartz 1932-2006
MELVIN SCHWARTZ 1932-2006 A Biographical Memoir by N. P. SAMIOS AND P. YAMIN © 2012 The National Academy of Sciences Any opinions expressed in this memoir are those of the authors and do not necessarily reflect the views of the National Academy of Sciences. MELVIN SCHWARTZ Courtesy of Brookhaven National Laboratories. November 2, 1932–August 28, 2006 BY N. P. SAMIOS AND P. YAMIN MEL SCHWARTZ DIED ON August 28, 2006, in Twin Falls, Idaho. He was born on 1 November 2, 1932, in New York City. He grew up in the Great Depression, but with a sense of optimism and desire to use his mind for the betterment of human- kind. He entered the Bronx High School of Science in the fall of 1945. It was there that his interest in physics began and that he recognized the importance of interactions with peers in determining his sense of direction in life. One of his classmates and future colleagues recalled that “even then” he wanted a Nobel Prize. Mel noted: My interest in physics began at the age of 12 when I entered the Bronx High School of Science. The four years I spent there were certainly among the most exciting and stimulating in my life, mostly because of the interaction with the other students of similar background, interest, and ability. MELVIN SCHWARTZ MELVIN On Sunday afternoons he attended a school run by the secular and Zionist Yiddish and many others. As Mel commented, “This faculty [was] at this time unmatched by any in the world, largely Nationaler Arbeter Farband (Jewish National Workers Alliance). -
01Ii Beam Line
STA N FO RD LIN EA R A C C ELERA TO R C EN TER Fall 2001, Vol. 31, No. 3 CONTENTS A PERIODICAL OF PARTICLE PHYSICS FALL 2001 VOL. 31, NUMBER 3 Guest Editor MICHAEL RIORDAN Editors RENE DONALDSON, BILL KIRK Contributing Editors GORDON FRASER JUDY JACKSON, AKIHIRO MAKI MICHAEL RIORDAN, PEDRO WALOSCHEK Editorial Advisory Board PATRICIA BURCHAT, DAVID BURKE LANCE DIXON, EDWARD HARTOUNI ABRAHAM SEIDEN, GEORGE SMOOT HERMAN WINICK Illustrations TERRY ANDERSON Distribution CRYSTAL TILGHMAN The Beam Line is published quarterly by the Stanford Linear Accelerator Center, Box 4349, Stanford, CA 94309. Telephone: (650) 926-2585. EMAIL: [email protected] FAX: (650) 926-4500 Issues of the Beam Line are accessible electroni- cally on the World Wide Web at http://www.slac. stanford.edu/pubs/beamline. SLAC is operated by Stanford University under contract with the U.S. Department of Energy. The opinions of the authors do not necessarily reflect the policies of the Stanford Linear Accelerator Center. Cover: The Sudbury Neutrino Observatory detects neutrinos from the sun. This interior view from beneath the detector shows the acrylic vessel containing 1000 tons of heavy water, surrounded by photomultiplier tubes. (Courtesy SNO Collaboration) Printed on recycled paper 2 FOREWORD 32 THE ENIGMATIC WORLD David O. Caldwell OF NEUTRINOS Trying to discern the patterns of neutrino masses and mixing. FEATURES Boris Kayser 42 THE K2K NEUTRINO 4 PAULI’S GHOST EXPERIMENT A seventy-year saga of the conception The world’s first long-baseline and discovery of neutrinos. neutrino experiment is beginning Michael Riordan to produce results. Koichiro Nishikawa & Jeffrey Wilkes 15 MINING SUNSHINE The first results from the Sudbury 50 WHATEVER HAPPENED Neutrino Observatory reveal TO HOT DARK MATTER? the “missing” solar neutrinos. -
Glossary of Terms Absorption Line a Dark Line at a Particular Wavelength Superimposed Upon a Bright, Continuous Spectrum
Glossary of terms absorption line A dark line at a particular wavelength superimposed upon a bright, continuous spectrum. Such a spectral line can be formed when electromag- netic radiation, while travelling on its way to an observer, meets a substance; if that substance can absorb energy at that particular wavelength then the observer sees an absorption line. Compare with emission line. accretion disk A disk of gas or dust orbiting a massive object such as a star, a stellar-mass black hole or an active galactic nucleus. An accretion disk plays an important role in the formation of a planetary system around a young star. An accretion disk around a supermassive black hole is thought to be the key mecha- nism powering an active galactic nucleus. active galactic nucleus (agn) A compact region at the center of a galaxy that emits vast amounts of electromagnetic radiation and fast-moving jets of particles; an agn can outshine the rest of the galaxy despite being hardly larger in volume than the Solar System. Various classes of agn exist, including quasars and Seyfert galaxies, but in each case the energy is believed to be generated as matter accretes onto a supermassive black hole. adaptive optics A technique used by large ground-based optical telescopes to remove the blurring affects caused by Earth’s atmosphere. Light from a guide star is used as a calibration source; a complicated system of software and hardware then deforms a small mirror to correct for atmospheric distortions. The mirror shape changes more quickly than the atmosphere itself fluctuates. -
Foundation Document Manhattan Project National Historical Park Tennessee, New Mexico, Washington January 2017 Foundation Document
NATIONAL PARK SERVICE • U.S. DEPARTMENT OF THE INTERIOR Foundation Document Manhattan Project National Historical Park Tennessee, New Mexico, Washington January 2017 Foundation Document MANHATTAN PROJECT NATIONAL HISTORICAL PARK Hanford Washington ! Los Alamos Oak Ridge New Mexico Tennessee ! ! North 0 700 Kilometers 0 700 Miles More detailed maps of each park location are provided in Appendix E. Manhattan Project National Historical Park Contents Mission of the National Park Service 1 Mission of the Department of Energy 2 Introduction 3 Part 1: Core Components 4 Brief Description of the Park. 4 Oak Ridge, Tennessee. 5 Los Alamos, New Mexico . 6 Hanford, Washington. 7 Park Management . 8 Visitor Access. 8 Brief History of the Manhattan Project . 8 Introduction . 8 Neutrons, Fission, and Chain Reactions . 8 The Atomic Bomb and the Manhattan Project . 9 Bomb Design . 11 The Trinity Test . 11 Hiroshima and Nagasaki, Japan . 12 From the Second World War to the Cold War. 13 Legacy . 14 Park Purpose . 15 Park Signifcance . 16 Fundamental Resources and Values . 18 Related Resources . 22 Interpretive Themes . 26 Part 2: Dynamic Components 27 Special Mandates and Administrative Commitments . 27 Special Mandates . 27 Administrative Commitments . 27 Assessment of Planning and Data Needs . 28 Analysis of Fundamental Resources and Values . 28 Identifcation of Key Issues and Associated Planning and Data Needs . 28 Planning and Data Needs . 31 Part 3: Contributors 36 Appendixes 38 Appendix A: Enabling Legislation for Manhattan Project National Historical Park. 38 Appendix B: Inventory of Administrative Commitments . 43 Appendix C: Fundamental Resources and Values Analysis Tables. 48 Appendix D: Traditionally Associated Tribes . 87 Appendix E: Department of Energy Sites within Manhattan Project National Historical Park . -
Letter of Interest Forthcoming Science from The
Snowmass2021 - Letter of Interest Forthcoming Science from the PROSPECT-I Data Set Neutrino Frontier Topical Groups: (NF02) Sterile neutrinos (NF03) Beyond the Standard Model (NF07) Applications (NF09) Artificial neutrino sources Contact Information: Nathaniel Bowden (LLNL) [[email protected]] Karsten Heeger (Yale University) [[email protected]] Pieter Mumm (NIST) [[email protected]] M. Andriamirado,6 A. B. Balantekin,16 H. R. Band,17 C. D. Bass,8 D. E. Bergeron,10 D. Berish,13 N. S. Bowden,7 J. P.Brodsky,7 C. D. Bryan,11 R. Carr,9 T. Classen,7 A. J. Conant,4 G. Deichert,11 M. V.Diwan,2 M. J. Dolinski,3 A. Erickson,4 B. T. Foust,17 J. K. Gaison,17 A. Galindo-Uribarri,12, 14 C. E. Gilbert,12, 14 C. Grant,1 B. T. Hackett,12, 14 S. Hans,2 A. B. Hansell,13 K. M. Heeger,17 D. E. Jaffe,2 X. Ji,2 D. C. Jones,13 O. Kyzylova,3 C. E. Lane,3 T. J. Langford,17 J. LaRosa,10 B. R. Littlejohn,6 X. Lu,12, 14 J. Maricic,5 M. P.Mendenhall,7 A. M. Meyer,5 R. Milincic,5 I. Mitchell,5 P.E. Mueller,12 H. P.Mumm,10 J. Napolitano,13 C. Nave,3 R. Neilson,3 J. A. Nikkel,17 D. Norcini,17 S. Nour,10 J. L. Palomino,6 D. A. Pushin,15 X. Qian,2 E. Romero-Romero,12, 14 R. Rosero,2 P.T. Surukuchi,17 M. A. Tyra,10 R. L. Varner,12 D. Venegas-Vargas,12, 14 P.B. -
Sc Ence Celebrating the Neutrino Number 25 1997
Los Alamos Sc ence Celebrating the Neutrino Number 25 1997 Celebrating the Neutrino . .1 The Evidence for Oscillations . .116 Bill Louis, Vern Sandberg, Gerry Garvey, Hywel White, Geoffrey Mills, and Rex Tayloe Reines-Cowan Experiments—Detecting the Poltergeist . .4 Neutrino oscillations are invoked as the explanation in experiments with solar, atmospheric, and accelerator- A compilation of papers and notes by Fred Reines and Clyde Cowan, Jr. produced (LSND) neutrinos. This summary of the experimental results for mixing angles and neutrino masses includes an interesting model that makes all three data sets consistent. The neutrino’s existence was inferred by Wolfgang Pauli in 1930, who feared that his clever construct might elude detection forever. Twenty-five years later, Fred Reines, Clyde Cowan, Jr., and a Los Alamos team detected the evasive particle. Their dedication to the chase and their innovative detection techniques set The Nature of Neutrinos in Muon Decay and Physics Beyond the Standard Model . .128 a precedent for all future neutrino experiments. Peter Herczeg Beta Decay and the Missing Energy . .7 Experiments that search for electron antineutrinos from m1-decay are sensitive not only to neutrino oscillations Fermi’s Theory of Beta Decay and Neutrino Processes . .8 but also to a class of muon decays that require leptonic interactions not present in the Standard Model. The author explores whether such decays could explain the observed excess of e1 events in the LSND experiments. The Oscillating Neutrino—An Introduction to Neutrino Masses and Mixing . .28 Exorcising Ghosts—In Pursuit of the Missing Solar Neutrinos . .136 Richard Slansky, Stuart Raby, Terry Goldman, and Gerry Garvey as told to Necia Grant Cooper Andrew Hime Today, the neutrino is at the center of particle physics as experimenters around the world explore the possibility that this tiny particle changes its identity just by moving between two points.